[0001] This invention relates to a transmitter for a communication device comprising: a
high-frequency power amplifier for amplifying the high-frequency signal to be transmitted,
which high-frequency power amplifier comprises an output stage for giving an amplified
high-frequency signal, and a measuring device for measuring the power of the high-frequency
signal, and to a mobile station which includes such a transmitter.
[0002] The transmitters of communication devices have a high frequency power amplifier,
in which the signal to be transmitted is amplified. The output of the high frequency
power amplifier is connected to the adapter circuit of the antenna, in which circuit
the impedance of the antenna is adapted to the output impedance of the high frequency
power amplifier. The purpose of the adaption is, among other things, to prevent the
formation of reflection waves from the antenna towards the high frequency power amplifier.
However, high frequency power amplifiers are sensitive to load variations. Load variations
cause distortion in the signal to be amplified, among other things. It is also possible
that the high frequency power amplifier is damaged in difficult load conditions. In
portable communication devices, in particular, the load variations of high frequency
power amplifiers are due to the interaction between the antenna and the operation
environment and changes in operating conditions. Metal objects in the vicinity of
the antenna, for example, can remarkably change the antenna impedance of the portable
communication device. This, in turn, has an effect on the operation point of the last
stage of the high frequency power amplifier, whereby the transistor is exposed to
large voltage and current variations. In time, these voltage and current variations
can impair the performance of the output stage transistor of the high frequency power
amplifier, and possibly also shorten its lifetime.
[0003] There are prior art solutions, in which the power signal formed by the high frequency
power amplifier is measured by means of a directional coupler and a detector diode.
For example, Figure 1 shows a prior art coupling, in which the directional coupler
DIR1 samples the power fed to the output. The samples are detected by a detector diode
D1. A method like this, based on a directional coupler, operates well when the load
impedance Z is constant. However, the method provides incorrect information in situations
in which the load impedance varies, as usually happens when portable communication
devices are used. In order to indicate this, the operation of the coupling in Figure
1 has been simulated. The simulation results can be seen in Figures 2a - 2e. In this
simulation, a bipolar transistor biased into the class AB was used as the power transistor
T1 of the output stage, and a harmonic trap was used to form the harmonics. Samples
of the output power were taken by a directional coupler DIR1, and the samples were
detected with a detector diode D1. The detector diode D1 was biased to the linear
region of operation, whereby the output power is proportional to the square of the
voltage V
meas formed by the detector diode D1.
[0004] Load variations are common in portable communication devices, such as mobile stations,
because the interaction between the environment and the antenna cause load variations
in the high frequency power amplifier. Table 1 shows various impedance values used
in the simulation. In the first simulation, the value of the load impedance Z was
such that it resulted in an optimum resistive load for the simulated amplifier. Different
values of the load impedance Z were used in other simulations, resulting in an incorrect
adaptation. The values used correspond to a reflection loss of -6 dB to a 6 ohm load.
Simulation results with different values of load impedance are shown in Figures 2a
- 2e. The power measurement was calibrated to produce the correct power reading with
an output power of two watts. Figures 2a - 2e show both the square of the voltage
V
meas formed by the detector diode D1 and the output power P
out of the amplifier in different load situations.
Table 1
Simulation no. |
Value of the load impedance Z |
1 |
6 Ω |
2 |
2 Ω |
3 |
18 Ω |
4 |
3.6+j4.8 Ω |
5 |
3.6-j4.8 Ω |
[0005] It can be seen from Figure 2a that the power measurement gives an accurate result
in optimum load conditions. It can further be seen from Figures 2b - 2e that when
the load of the amplifier varies, the square of the detected voltage is no more the
same as the power conveyed to the load, whereby the measurement does not give the
correct idea of the load situation of the amplifier.
[0006] Still another disadvantage of using a directional coupler is the fact that a directional
coupler causes power loss in the signal to be transmitted. In practical applications,
the directional coupler is typically implemented by means of conductor traces incorporated
directly on the printed circuit board (PCB), whereby the power loss of the directional
coupler is typically approx. 0.5 dB. In addition, a directional coupler formed directly
on the circuit board takes an unnecessarily large amount of space.
[0007] Measurement of the signal power is used to adjust the output power of high frequency
transmitters. It is an aim of the present invention to reduce the disadvantages presented
above and to achieve a device for adjusting the power in the power amplifier of the
transmitter of a communication device, and a mobile station in which the invention
can be advantageously applied. The invention is based on the idea that voltage and
current are measured at the output stage of the high frequency power amplifier, whereby
the load impedance at the output stage can be calculated and the transmission power
adjusted accordingly. The transmitter according to the invention is characterized
in what is put forth in the characterizing part of Claim 1. A mobile station according
to the invention is characterized in what is put forth in the characterizing part
of Claim 9.
[0008] In a preferred embodiment of the invention, the output stage comprises a transmitter
according to Claim 1, characterized in that the output stage comprises an amplification
means, in which the high-frequency signal is arranged to be amplified. Optionally,
the output stage includes means for calculating the power of the high-frequency signal
on the basis of the measured high-frequency voltage and high-frequency current.
[0009] The present invention has many advantages compared to prior art transmitters and
mobile stations. Preferably, the high frequency current running through the amplifier
and the high frequency voltage at the output of the amplifier are measured, whereby
the load impedance can be calculated very accurately and the output stage can be adjusted
on the basis of this to the optimum point of operation. The high-frequency current
and the high-frequency voltage are measured as close to the output of the last stage
as possible, whereby potential transmission line losses and other losses having an
effect on the measurement results can be eliminated and the reliability of the measurements
improved compared to the measurements of prior art technique. In addition, it is possible
to find out the real load during the transmission, which has an effect on the transistor
of the output stage, and thereby to improve the adjustment of the optimum point of
operation of the transistor in varying operating conditions. The efficiency of the
transmitter according to the present invention is improved as compared to the prior
art transmitters, because the measurement of high-frequency current and voltage does
not cause a substantial power loss in the output signal. Due to better efficiency,
the output power of the transmitter can be somewhat reduced. The measurement coupling
can also be implemented in a small space by integrating it to the same semiconductor
chip as the power transistor of the output stage of the power amplifier. Space is
also saved on the circuit board, and the size of communication devices can be reduced.
Potential variations of the load impedance are also taken into account in the measurements
according to the invention, which also increases the reliability of the measurement.
[0010] In the following, the invention will be described in more detail with reference to
the accompanying drawings, in which
- Figure 1
- shows a prior art power measurement,
- Figures 2a-2e
- show the simulation results of circuit in Figure 1,
- Figure 3
- shows a measurement coupling according to the first embodiment of the invention,
- Figures 4a-4e
- show the simulation results of the circuit and calculated output powers for the coupling
in Figure 3 with various load impedances,
- Figures 5a-5e
- show voltages measured and calculated for the coupling in Figure 3 over the collector-emitter
junction with various values of the load impedance,
- Figures 6a-6e
- show the measured and calculated emitter currents of the transistor with various values
of the load impedance,
- Figures 7a-7e
- show estimation results of the transistor load impedance in the coupling shown in
Figure 3,
- Figure 8
- shows another preferred embodiment of the invention, and
- Figure 9
- shows a mobile station according to the invention.
[0011] The block diagram of Figure 3 shows the output stage and measurement circuit of a
transmitter according to the first embodiment of the invention. A transistor T1 or
other amplifying component can be advantageously used as the amplifying element of
the output stage. The high-frequency signal to be transmitted is directed to the pin
P
in. The high-frequency signal is further conveyed through the first capacitor C1 for
amplification at the base of the transistor T1 of the output stage. The transistor
T1 can be, for example, a bipolar transistor, which has sufficient power capability
and high frequency properties in the application used at the time. The point of operation
of the transistor T1 is set correct by means of a basing voltage conveyed to the base
of the transistor T1. The biasing voltage is formed by a biasing voltage source U
bias and conveyed via the first choke L1. The biasing voltage U
bias can be formed with a voltage division coupling implemented with resistors, for example,
and it is a technique well known to a person skilled in the art.
[0012] The high-frequency signal to be transmitted, directed to the base of the transistor
T1, is amplified in the transistor T1, whereby an amplified, high-frequency output
signal is received from the collector, which signal is directed via a second capacitor
C2 to the load impedance Z. The load impedance Z preferably comprises an antenna and
adapting means for achieving an optimum adaptation between the collector circuit and
the antenna. In addition, the adapting circuit can comprise a band-pass filter, which
is used to attenuate spurious transmissions.
[0013] The operating voltage needed by the transistor T1 is directed to the collector of
the transistor T1 via a second choke L2.
[0014] The emitter circuit of the transistor T1 preferably comprises a resistor R1 and an
earth stray inductance L3.
[0015] The high-frequency alternating voltage of the collector-emitter junction of the transistor
T1 is preferably sensed in a manner such that a voltage signal is directed via a third
capacitor C3 to the positive input line of the first differential amplifier A1, and
the alternating voltage of the emitter of the transistor T1 is directed via the fourth
capacitor C4 to the negative input line of the first differential amplifier A1. Thus
a voltage V
rf proportional to the high-frequency collector emitter voltage V
CE is received from the output of the first differential amplifier A1.
[0016] A voltage proportional to the high-frequency emitter current I
E of the transistor T1 can be sensed by differential amplifier A2 through the capacitors
C4 and C5.
[0017] In the first rectifier RECT1, an absolute value |V
rf| is formed from the signal V
rf proportional to the voltage, and integrated in the first integrator INT1, resulting
in a voltage V
meas, which is proportional to the mean of the collector-emitter voltage of the transistor
T1. The absolute value |I
rf| of the voltage I
rf proportional to the emitter current is formed in the second rectifier RECT2. The
rectified voltage is further integrated in a second integrator INT2, whereby a voltage
I
meas proportional to the mean value of the emitter current is received from the output
of the second integrator.
[0018] The real average power of the transistor T1 can be determined by multiplying the
voltage by the current value. In the circuit shown in Figure 3 this has been implemented
by directing the output signal of the first differential amplifier A1 and the output
signal of the second differential amplifier A2 to the multiplier circuit M1. The multiplier
circuit M1 forms a signal proportional to each instantaneous power, which signal is
integrated in the third integrator INT3 for forming a voltage P
dc proportional to the mean value of the real power.
[0019] The measurements according to the invention are formed from signals as near to the
power transistor T1 of the output stage as possible, whereby possible transmission
line losses and other losses having an effect on the measurement results can be eliminated
and the reliability of the measurements improved as compared to the prior art measurements.
In addition, it is easier to find out the real load on the transistor of the output
stage during the transmission, whereby the adjustment of the optimum operation point
of the transistor becomes more accurate in varying operating conditions.
[0020] Figures 4a - 4e show some simulation results with the simulation coupling of a preferred
embodiment of the invention according to Figure 3. In the figures, a dashed line depicts
the measured output power P
dc, and a solid line a theoretical, calculated output power P
out on the basic frequency. The powers have been shown as a function of the input power
P
in. The difference between the figures is the load impedance Z used in the simulation,
the values of which in different simulations are as shown in Table 1. It can be clearly
seen from the figures that both the measured and the calculated power are close to
each other. The differences are mainly due to the fact that the measured power P
dc is the total power, inclusive of the harmonic frequencies, which are not included
in the theoretical power value P
out.
[0021] As was mentioned above in connection with the description of the coupling shown in
Figure 3, the high frequency currents and voltages of the transistor T1 are also measured
in addition to the power. The measurements of the voltages and currents of the transistor
are of great importance with regard to the maintenance of optimum operation conditions
of the transistor. In power transistors, in particular, the load variations have a
direct effect as variations of currents and voltages. Strong variations of voltage
and current cause distortion in the signal and can even destroy the transistor.
[0022] An example of a situation in which strong voltage and current variations can be formed
in the power transistor is when a mobile station without an accumulator is connected
to a charging device, and the antenna is possibly carelessly set on its place. In
a transmitter according to the present invention, the voltage and current measurement
information can be used to adjust the operation point of the transistor, whereby the
signal is distorted less and the destruction of the transistor of the output stage
can be avoided.
[0023] Another example in which large voltage and current variations are possible is a situation
in which a bipolar transistor is loaded with a load of a small impedance. Very strong
current variations are then formed in the transistor, and in the long run these variations
reduce the reliability of the transistor. In these situations, the measurement method
according to the invention also prevents the disadvantages mentioned.
[0024] Figures 5a - 5e show both the theoretical and the measured voltage values of the
collector-emitter junction of the transistor in a coupling according to Figure 3.
In the figures, a solid line is used to depict the calculated RMS value V
calc of the high-frequency voltage of the collector-emitter junction of the transistor
T1. A dashed line is used to depict a rectified and low-pass filtered voltage V
meas, which is a good estimate of the high-frequency voltage of the collector-emitter
junction of the transistor T1. Corresponding measurement results could also be formed
by using a peak detector instead of a rectifier RECT1. It can be seen from the figures
5a - 5e that the measured values very accurately correspond to the calculated values,
which means that the measurement is very reliable. It can also be seen from the figures
that with loads that are active and have a high impedance, the collector-emitter voltage
of the transistor increases as compared to the optimum, resistive load of 6 Ω.
[0025] Similarly, the simulation results of the high-frequency emitter current of the transistor
T1 have been shown in Figures 6a - 6e, in which a solid line is used to depict the
calculated current I
calc, and a dashed line is used to depict the measured current I
meas. The impedance values used are the same as in the previous figures, in accordance
with Table 1. Large current variations can be seen in Figure 6b, where the impedance
used was a resistive load of 2 Ω, and in Figure 6e, where the load impedance was 3.6
+ 4.8 Ω.
[0026] A further advantage of the invention is the fact that the measurement results of
the high-frequency current and voltage can be used to estimate the real load impedance
of the output stage transistor T1. The absolute value of the load impedance is proportional
to the relationship between the measured voltage and current: V
meas/I
meas, and the term cos (Φ) is proportional to the formula

. These results are shown in the figures 7a - 7e.
[0027] The blocks of the block diagram of the preferred embodiment of the invention according
to Figure 3 are well known, and numerous examples of them are found in the literature
dealing with this technology.
[0028] In some practical applications, the transistor T1 of the output stage can be implemented
by means of several parallelly connected transistors for achieving a sufficient output
power. Then the voltage is measured as described above, and the current is measured
at the emitter of one of the transistors. In this case, the current measurement result
must be multiplied by the number of the parallelly connected transistors. This can
preferably be implemented in a manner such that the amplification of the second differential
amplifier A2 is set correspondingly; for example, when three transistors are used,
the amplification is set as triple compared to an application implemented by one transistor.
[0029] Figure 8 shows a second preferred embodiment of the invention as a simplified block
diagram. The difference compared to the embodiment shown in Figure 3 is primarily
that the current measurement is carried out by means of a second resistor R2 connected
to the output line of the output stage. The voltage and current measurement results
are dealt with as has been described in connection with the embodiment of Figure 3.
[0030] Current sensing is also possible using other current sensors such as transformers.
As was already mentioned above, peak detectors can be used in place of rectifiers
RECT1, RECT2.
[0031] The measurements described above should be placed as near to the power transistor
T1 of the output stage as possible, whereby the measurement coupling is preferably
integrated to the same semiconductor chip as the power transistor. Among other things,
this has the advantage that the transmission paths of the signals can be made as short
as possible, which reduces the interaction between the signal paths. In applications
in which the frequencies of the high-frequency signals used are not very high, separate
components can also be used to implement the measurement coupling.
[0032] Figure 9 shows a mobile station 1 according to the present invention as a simplified
block diagram. The mobile station 1 can be, for example, a GSM mobile station. In
the modulation block 3 of the transmitter 2 a high-frequency signal is formed, to
which the signal transmitted thereto, such as the signal of the microphone 11, has
been modulated. The high-frequency signal is directed to the pin P
in of the output stage 4. In this example, the output stage 4 corresponds to an output
stage according to Figure 3. The high-frequency signal is further directed via the
first capacitor C1 to the base of the transistor T1 of the output stage for amplification.
The transistor T1 can be, for example, a bipolar transistor, which has sufficient
power endurance and high frequency properties for the application used at the time.
The operating point of the transistor T1 is set correct by means of a basing voltage
directed to the base of the transistor T1. The biasing voltage is formed by the biasing
voltage source U
bias and conveyed via the first choke L1.
[0033] The high-frequency signal to be transmitted and conveyed to the base of the transistor
T1 is amplified in the transistor T1, whereby an amplified, high-frequency output
signal is received from the collector, which signal is directed via a second capacitor
C2 to the load impedance Z. The load impedance preferably comprises an antenna and
adapting means for achieving an optimum adaptation between the collector circuit and
the antenna. In addition, the adaptation circuit can comprise a band-pass filter,
which is used to attenuate spurious transmissions.
[0034] The operating voltage needed by the transistor T1 is directed to the collector of
the transistor T1 via a second choke L2.
[0035] The emitter circuit of the transistor T1 preferably comprises a resistor R1 and an
earth stray inductance L3.
[0036] The high-frequency alternating voltage of the collector-emitter junction of the transistor
T1 is preferably measured in a manner such that a voltage signal is directed from
the collector via a third capacitor C3 to the positive input line of the differential
amplifier A1, and the alternating voltage of the emitter of the transistor T1 is directed
via the fourth capacitor C4 to the negative input line of the first differential amplifier
A1. Thus a voltage V
rf, proportional to the high-frequency collector-emitter voltage V
CE, is received from the output of the first differential amplifier A1.
[0037] The high-frequency emitter current I
E of the transistor T1 can be determined by measuring the voltage over the resistor
R1, as has been described above in connection with the description of Figure 3. This
voltage is measured by directing the emitter voltage of the transistor via the fourth
capacitor C4 to the negative input line of the second differential amplifier A2, and
the voltage on the side of the earth stray inductance of the resistor R1 via the fifth
capacitor C5 to the positive input line of the second differential amplifier A2. Thus
the second differential amplifier A2 forms a voltage signal proportional to the emitter
current of the transistor T1, which signal is here denoted by I
rf.
[0038] In the first rectifier RECT1, an absolute value |V
rf| is formed from the signal V
rf, proportional to the voltage, and integrated in the first integrator INT1, resulting
in a voltage V
meas proportional to the mean value of the collector-emitter voltage of the transistor
T1. An absolute value |I
rf| is formed in the second rectifier RECT2 from the voltage I
rf proportional to the emitter current. The rectified voltage is further integrated
in the second integrator INT2, whereby a voltage I
meas, proportional to the mean value of the emitter current, is received from the output
of the second integrator.
[0039] The real average power formed by the transistor T1 is found out by multiplying the
voltage values by the current values advantageously in a manner such that the output
signal of the first differential amplifier A1 and the output signal of the second
differential amplifier A2 are directed to a multiplier circuit M1, such as a mixer.
The multiplier circuit M1 forms a signal proportional to each instantaneous power,
which signal is integrated in the third integrator INT3 for forming a voltage P
dc proportional to the mean value of the real power.
[0040] The measurement results are converted by analog-to-digital converters 5a, 5b, 5c
to digital form and directed to the control unit 6 of the mobile station, such as
a microcontroller. The application software of the control unit 6 includes a program
in which the measurement results are processed in order to determine, among other
things, whether the transmission power must be reduced due to a change in the load
impedance of the output stage 4, for example.
[0041] If the transmission power must be adjusted, the control unit 6 forms an adjustment
signal for the modulation block 3 of the transmitter, whereby the power of the output
signal of the modulation block 3 is reduced, which in turn reduces the output power
of the output stage 4.
[0042] From the output stage 4, the amplified high-frequency signal is directed via a duplex
filter 7 to the antenna 8. A certain frequency band is reserved for the use of each
mobile station system. This frequency band is usually divided into uplink and downlink
frequency bands, which means that the transmission of the mobile station 1 to the
base station (not shown) takes place at a different frequency from the base station
transmission to the mobile station 1. The duplex filter 7 includes a first band-pass
filter 7a, the passband of which comprises the transmission frequency band of the
mobile station system, and a second band-pass filter 7b, the passband of which comprises
the reception frequency band of the mobile station system. Thus the high-frequency
signals from the transmitter do not disturb the operation of the receiver, because
they do not substantially pass through the second band-pass filter 7b.
[0043] The high-frequency signals to be received are directed from the antenna 8 via the
second band-pass filter 7b of the duplex filter 7 to the receiver 9, which is, for
example, a prior art mobile station receiver. In the receiver 9, the received signal
is demodulated and directed to the earphone 12.
[0044] The local oscillator frequencies of the transmitter 2 and the receiver 9 are generated
by the local oscillator 10, the frequency of which is controlled by the controller
6. The mobile station 1 in Figure 9 also comprises a keypad 13 and a display 14.
[0045] The present invention is not limited to the above described embodiments only, but
it can be modified within the scope defined by the attached claims.
1. A transmitter for a communication device comprising:
- a high-frequency power amplifier for amplifying the high-frequency signal to be
transmitted, which high-frequency power amplifier comprises an output stage for giving
an amplified high-frequency signal, and
- a measuring device for measuring the power of the high-frequency signal, characterized
in that the measuring device comprises means for measuring the voltage and current
of the high-frequency signal in said output stage, and means for calculating the power
of the high-frequency signal on the basis of the measured high-frequency voltage and
high-frequency current.
2. A transmitter according to Claim 1, characterized in that it comprises a load impedance,
to which the amplified high-frequency signal is arranged to be directed, and means
for calculating the load impedance on the basis of the measured high-frequency voltage
and high-frequency current.
3. A transmitter according to Claim 1 or Claim 2, characterized in that the output stage
comprises an amplification means, in which the high-frequency signal is arranged to
be amplified.
4. A transmitter according to Claim 3, characterized in that the amplification means
of the output stage is implemented by one transistor, whereby the high-frequency voltage
is arranged to be measured between the collector and emitter of the transistor and
the high-frequency current is arranged to be measured at the emitter circuit of the
transistor.
5. A transmitter according to Claim 3, characterized in that the amplification means
of the output stage is implemented by two or more transistors, whereby the high-frequency
voltage is arranged to be measured between the collector and emitter of the transistor
and the high-frequency current is arranged to be measured at the emitter circuit of
one transistor, and the amplification of the second differential amplifier is preferably
arranged as proportional to the number of transistors used in the amplification means.
6. A transmitter according to any of Claims 1 to 5, characterized in that
- the high-frequency voltage measuring device comprises a first differential amplifier
for forming a measurement signal proportional to the high-frequency collector-emitter
voltage, a first rectifier for forming the absolute value of the measurement signal
proportional to the collector-emitter voltage, and a first integrator for forming
a measurement signal proportional to the mean value of the collector-emitter voltage
of the transistor,
- the high-frequency current measuring device comprises a second differential amplifier
for forming a measurement signal proportional to the high-frequency emitter current,
a second rectifier for forming the absolute value proportional to the emitter current
and a second integrator for forming a measurement signal proportional to the mean
value of the emitter current of the transistor, and
- the measuring device of the high-frequency power comprises a multiplier circuit
for forming a measurement signal proportional to each instantaneous power by multiplying
the high-frequency measurement signal proportional to the collector-emitter voltage
by the high-frequency measurement signal proportional to the emitter current for forming
a measurement signal proportional to the mean value of the power of a third integrator.
7. A transmitter according to Claim 6, characterized in that the measurement signals
are analog signals.
8. A transmitter according to any of Claims 1 to 7, characterized in that the measurement
signals are arranged to be used for adjusting the operating point of the output stage.
9. A mobile station, which includes a transmitter for transmitting signals, which transmitter
comprises
- a high-frequency amplifier for amplifying the high-frequency signal to be transmitted,
which high-frequency power amplifier includes an output stage for giving an amplified
high-frequency signal, and
- a measuring device for measuring the power of the high-frequency signal, characterized
in that the measuring device comprises means for measuring the voltage and the current
in said output stage, and means for calculating the power of the high-frequency signal
on the basis of the measured high-frequency voltage and high-frequency current.
10. A mobile station according to Claim 9, characterized in that it is a GSM mobile station.